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Volumn 55, Issue 4, 1997, Pages 3958-3961

Microscopic nonuniversality versus macroscopic universality in algorithms for critical dynamics

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EID: 0000872561     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.55.3958     Document Type: Article
Times cited : (13)

References (33)
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    • See,) for a recent review on phase-ordering kinetics after quenches to low temperatures
    • See, A J. Bray, Adv. Phys.43, 357 (1994) for a recent review on phase-ordering kinetics after quenches to low temperatures.
    • (1994) Adv. Phys. , vol.43 , pp. 357
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    • University of Siegen, Si-95-07, and, Report, (unpublished)
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    • Okano, K.1    Schülke, L.2    Yamagishi, K.3    Zheng, B.4
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    • J. Phys. A28, L639 (1995);
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    • (private communication)
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    • K. Binder and D. W. Heermann, Monte Carlo Simulation in Statistical Physics, (Springer, Berlin, 1988) provides a good introduction to the dynamic interpretation of Monte Carlo simulations and the different algorithms used
    • K. Binder and D. W. Heermann, Monte Carlo Simulation in Statistical Physics, (Springer, Berlin, 1988) provides a good introduction to the dynamic interpretation of Monte Carlo simulations and the different algorithms used.
  • 32
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    • For descriptions of the heat-bath algorithm, see, and, and, For the MC simulations reported in the present work the heat-bath algorithm is equivalent to the original Glauber dynamics, see, and
    • For descriptions of the heat-bath algorithm, see B. Derrida and G. Weisbuch, Europhys. Lett.4, 657 (1987) and A. M. Mariz, H J. Herrmann and L. de Arcangelis, J. Stat. Phys.59, 1043 (1990). For the MC simulations reported in the present work the heat-bath algorithm is equivalent to the original Glauber dynamics, see A M. Mariz and H J. Herrmann, J. Phys. A22, L1081 (1989).
    • (1989) J. Phys. A , vol.22
    • Derrida, B.1    Weisbuch, G.2    Mariz, A.M.3    Herrmann, H.J.4    de Arcangelis, L.5    Mariz, A.M.6    Herrmann, H.J.7
  • 33
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    • For a detailed discussion of the later stages, especially the time scales which determine the location of the maximum and the rate of decay to the equilibrium, we refer to Refs. 5,12
    • For a detailed discussion of the later stages, especially the time scales which determine the location of the maximum and the rate of decay to the equilibrium, we refer to Refs. 5,12.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.